Electrical junction

ABSTRACT

An electrical junction comprising a first pair of leads and a second pair of leads. The first pair of leads and the second pair of leads comprise a Weyl semimetal. The junction comprises an electrical crossing arranged between the leads of the first pair and the leads of the second pair and is configured to provide an electrical connection between the leads of the first pair and the leads of the second pair. A related electrical device and a related neural network may be also presented.

BACKGROUND

Aspects of the present invention relate generally to electricaljunctions arranged between electrical conductors.

Further aspects relate to electrical devices comprising electricaljunctions and neural networks comprising electrical junctions.

Neural networks are widely used in pattern recognition andclassification, with many potential applications. The parameters (e.g.,‘synaptic weights’) of the neural network may be adaptively trained on aset of patterns during a learning process, following which the neuralnetwork is able to recognize or classify patterns of the same kind.

Neural network applications may include pattern recognition,classification, and identification of fingerprints, faces, voiceprints,similar portions of text, similar strings of genetic code, prediction ofthe behavior of systems etc.

Hardware implementations of neural network architectures require amultitude of interconnects to connect all outputs of neurons from onelayer to the inputs of neurons from the next layer. The number of suchconnections may be very large in preferred systems. Their physicalimplementation is challenging because current hardware fabricationrelies mostly on 2D fabrication techniques. However, with such 2Dfabrication techniques the signal lines cannot be crossed withoutcreating a shortcut. Also multi-layer CMOS implementations with severalmetal layers have limited capabilities to solve this issue.

Accordingly, it is generally desirable to provide other electricaljunctions, in particular electrical junctions that facilitate anintegration of crossings between electrical wires with high density.

SUMMARY

According to a first aspect, the invention is embodied as an electricaljunction comprising a first pair of leads and a second pair of leads.The first pair of leads and the second pair of leads comprise a Weylsemimetal. The junction comprises an electrical crossing arrangedbetween the leads of the first pair and the leads of the second pair andis configured to provide an electrical connection between the leads ofthe first pair and the leads of the second pair.

The leads may be in particular electrical wires. The electricalcrossing, which may also be denoted as electrical node, provides anelectrical connection between the leads of the first pair and the leadsof the second pair. In other words, the electrical crossing isunderstood as the central part of the junction at which the leadsconverge and at which they are electrically connected with each other.

According to embodiments, the Weyl semimetal of the leads of the firstpair is magnetized in a first magnetization direction and the Weylsemimetal of the leads of the second pair is magnetized in a secondmagnetization direction. The second magnetization direction is differentfrom the first magnetization direction.

While the Weyl-semimetal of the first pair of leads and theWeyl-semimetal of the second pair of leads are magnetized in differentmagnetization directions, the electrical crossing is not magnetized.

An overview of the current research on Weyl semimetals is provided byShuang Jia, Su-Yang Xu and M. Zahid Hasan Weyl in the document “Weylsemimetals, Fermi arcs and chiral anomalies”, 1140 NATURE MATERIALS, VOL15, NOVEMBER 2016. According to this document “Weyl semimetals aresemimetals or metals whose quasiparticle excitation is the Weyl fermion,a particle that played a crucial role in quantum field theory, but hasnot been observed as a fundamental particle in vacuum. Weyl fermionshave definite chiralities, either left-handed or right-handed. In a Weylsemimetal, the chirality can be understood as a topologically protectedchiral charge. Weyl nodes of opposite chirality are separated inmomentum space and are connected only through the crystal boundary by anexotic non-closed surface state, the Fermi arcs. Weyl fermions arerobust while carrying currents, giving rise to exceptionally highmobilities. Their spins are locked to their momentum directions, owingto their character of momentum-space magnetic monopole configuration.Because of the chiral anomaly, the presence of parallel electric andmagnetic fields can break the apparent conservation of the chiralcharge, making a Weyl metal, unlike ordinary nonmagnetic metals, moreconductive with an increasing magnetic field.”

Embodiments of the invention may facilitate cost-efficient massfabrication of electrical junctions. Furthermore, electrical junctionsaccording to embodiments of the invention may provide low poweroperation and high integration densities.

According to an embodiment the first pair of leads and the second pairof leads are configured to transport Weyl-fermions. The Weyl-fermionsmay be in particular embodied as electronic excitations.

Hence according to such an embodiment electrical signals that shall betransferred between the two leads of the first pair or between the twoleads of the second pair are represented by Weyl-fermions.

The first magnetization direction is parallel to a direction ofpropagation of the Weyl-fermions in the first pair of leads and thesecond magnetization direction is antiparallel to the direction ofpropagation of the Weyl-fermions in the second pair of leads.

Central part of junction can be a Weyl material or another conductivematerial (metal/semiconductor) which does not lead to scattering of thecarriers.

Hence embodiments of the invention exploit the topologically protectedtransport of Weyl fermions inside the Weyl semimetals in order to reduceor minimize a cross coupling of the electrical signal that shall betransported between the leads of the first pair into the leads of thesecond pair during its transport through the crossing. Likewise,embodiments of the invention exploit the ballistic, but topologicallyprotected transport of Weyl fermions inside the Weyl semimetals in orderto reduce or minimize a cross coupling of the electrical signal thatshall be transported between the leads of the second pair into the leadsof the first pair during its transport through the crossing.

According to embodiments, the first pair of leads is configured totransport Weyl-fermions of a first chirality and the second pair ofleads is configured to transport Weyl-fermions of a second chirality.The first chirality may be in particular a right-handed chirality andthe second chirality may be in particular a left-handed chirality.

The first pair of leads comprises a plurality of first magnetizedelements being configured to apply a directed magnetic field in thefirst magnetization direction on the Weyl-semimetal of the first pair ofleads and the second pair of leads comprises a plurality of magnetizedelements being configured to apply a directed magnetic field in thesecond magnetization direction on the Weyl-semimetal of the second pairof leads.

According to embodiments, the plurality of first magnetized elements andthe plurality of second magnetized elements are arranged adjacent to theWeyl-semimetal of the first pair of leads and adjacent to the Weylsemimetal of the second pair of leads respectively.

This allows for an efficient application of magnetic fields on theWeyl-semimetal. The attachment of the first and the second magnetizedelements to the Weyl-semimetal may be performed with fabrication methodsknown to a skilled person in the art such as e.g. gluing, metaldeposition through a mask, lithography processes, and self-assemblyprocesses.

According to embodiments, the plurality of first magnetized elements areembodied as magnetized layers and/or the plurality of second magnetizedelements are embodied as magnetized layers.

According to embodiments, the plurality of first magnetized elements areembedded in the Weyl semimetal of the first pair of leads and theplurality of second magnetized elements are embedded in the Weylsemimetal of the second pair of leads. This allows for an efficientapplication of magnetic fields on the Weyl-semimetal. SuchWeyl-semimetals with embedded magnetized elements may be fabricated withfabrication methods known to a skilled person in the art such as e.g.doping with magnetic elements during the crystal growth of the Weylsemimetal or placing a magnetic film in proximity.

According to embodiments, the plurality of first magnetized elementsand/or the plurality of second magnetized elements comprise rare earthmagnets.

According to further embodiments, the plurality of first magnetizedelements and/or the plurality of second magnetized elements comprise amaterial selected from the group consisting of Neodymium-iron-boron,manganese aluminum, samarium cobalt and aluminum nickel cobalt.

According to embodiments, the Weyl-semimetal may be in particular TaAs,NbP or TaP. According to other embodiments, the Weyl semimetal may beRPtBi or GdPtBi. These materials turn into a Weyl semimetal by applyinga magnetic field B.

According to other embodiments, the Weyl-semimetal may be a Dirac metal.The Dirac metal may be in particular Cd₂As₃ or Na₃Bi. Such Dirac metalsturn into a Weyl semimetal by the application of a magnetic field B.

According to embodiments, a crossing angle between the leads of thefirst pair and the leads of the second pair is less than 30 degree, inparticular less than 20 degree.

Such embodiments further reduce or minimize the cross coupling of anelectrical signal of one of the pair of leads into the other pair ofleads.

According to embodiments, the crossing is configured to provide adistance, which may also be denoted as transport length, between theleads of the first pair that is sufficiently small to keep the firstchirality of the Weyl-fermions during their transport through thecrossing and to provide a distance (transport length) between the leadsof the second pair that is sufficiently small to keep the secondchirality of the Weyl-fermions during their transport through thecrossing.

While in the leads of the first pair and the leads of the second pairthe respective chirality is maintained or in other words enforced or inother words supported by the corresponding magnetization of the leads,such a maintenance, enforcement or support is missing during thetransport of the Weyl-fermions through the crossing due to an absence ofa corresponding magnetic field in the crossing. But by providing limitedphysical dimensions e.g. ensuring ballistic, scattering-free transport,of the crossing and thereby limiting the distance that the Weyl-fermionshave to travel between the respective leads without magnetizationsupport, the respective chirality of the Weyl-fermions can be keptnevertheless.

According to embodiments, the crossing is configured to provide adistance between the leads of the first pair and the leads of the secondpair between 50 nm and 300 nm.

According to embodiments, the crossing comprises a non-magnetizedWeyl-semimetal.

According to an embodiment of another aspect of the invention, anelectrical device comprising a plurality of junctions according to thefirst aspect is provided. This is in particular advantageous forelectrical devices with a large number of electrical connections andcorresponding crossings.

According to an embodiment of another aspect of the invention, a neuralnetwork is provided. The neural network comprises a plurality ofneurons, a plurality of connections between the neurons and a pluralityof junctions according to first aspect. The plurality of junctions isconfigured to provide a plurality of crossings between the pluralitiesof connections.

Embodiments of the invention will be described in more detail below, byway of illustrative and non-limiting examples, with reference to theaccompanying drawings.

BRIEF DESCRIPTION OF THE SEVERAL VIEWS OF THE DRAWINGS

FIG. 1 shows a schematic view of a neural network according to anembodiment of the invention;

FIG. 2 shows a more detailed view of a part of a neural networkaccording to an embodiment of the invention;

FIG. 3 illustrates a signal flow of an electrical signal in a first pairof leads of an electrical junction according to an embodiment of theinvention;

FIG. 4 illustrates a signal flow of an electrical signal in a secondpair of leads of an electrical junction according to an embodiment ofthe invention;

FIG. 5 shows an electrical junction according to an embodiment of theinvention comprising magnetized elements adjacent to a Weyl-semimetal;

FIG. 6 shows an electrical junction according to an embodiment of theinvention comprising magnetized elements embedded in a Weyl-semimetal;

FIG. 7 shows a top view of an electrical junction according to anembodiment of the invention having a layer of magnetized elements on topof the Weyl-semimetal;

FIG. 8a shows a corresponding cross-sectional view of a first pair ofleads and a crossing taken along the section line I-I of FIG. 7;

FIG. 8b shows a corresponding cross-sectional view of a second pair ofleads and the crossing taken along the section line II-II of FIGS. 7;and

FIG. 9 shows a cross-sectional view of another embodiment taken alongthe section line I-I of FIG. 7, comprising a vertical junction.

DETAILED DESCRIPTION

FIG. 1 shows a schematic view of a neural network 100 according to anembodiment of the invention. The neural network 100 comprises an inputlayer 110 comprising a plurality of neurons 10, two hidden layers 120comprising a plurality of neurons 10 and an output layer 130 comprisinga plurality of neurons 10. The neural network 100 comprises a pluralityof electrical connections 20 between the neurons 10. The electricalconnections 20 connect the outputs of neurons from one layer, e.g. fromthe input layer110, to the inputs of neurons from the next layer, e.g.one of the hidden layers 120. As illustrated in FIG. 1, the number ofsuch connections 20 may be very large.

FIG. 2 shows a more detailed view of a part of a neural network 200according to an embodiment of the invention. The neural network 200comprises four neurons 10 a, 10 b, 10 c and 10 d. The two upper neurons10 a and 10 b and the two lower neurons 10 c and 10 d are connected byelectrical connections 20 a which have no crossings with otherelectrical connections. The upper neuron 10 a and the lower neuron 10 das well as the lower neuron 10 c and the upper neuron 10 b are connectedby electrical connections 20 b which cross each other at a crossing 30.The crossing 30 forms a central point of an electrical junction 40.

FIG. 3 and FIG. 4 show an enlarged view of the electrical junction 40 ofFIG. 2 and illustrates the desired signal flow of the electricaljunction 40.

The electrical junction 40 comprises a first pair of leads comprising alead 50 a and a lead 50 b. Furthermore, the electrical junction 40comprises a second pair of leads comprising a lead 51 a and a lead 51 b.The leads 50 a, 50 b as well as the leads 51 a and 51 b each comprise aWeyl semimetal 55. The electrical crossing 30 is arranged between theleads 50 a, 50 b of the first pair and the leads 51 a, 51 b of thesecond pair. The electrical crossing 30 provides an electricalconnection between the leads 50 a, 50 b as well as between the leads 51a and 51 b.

The Weyl semimetal 55 of the leads 50 a, 50 b of the first pair ismagnetized in a first magnetization direction 60 and the Weyl semimetal55 of the leads 51 a, 51 b of the second pair is magnetized in a secondmagnetization direction 61.

The Weyl semimetal 55 is a new state of matter that hosts Weyl fermionsas emergent quasiparticles and admits a topological classification thatprotects Fermi arc surface states on the boundary of a bulk sample. Weylsemimetals have an unusual band structure in which the linearlydispersing valence and conduction bands meet at discrete “Weyl points.”

According to some embodiments, the Weyl-semimetal 55 may comprise TaAs,NbP or TaP.

According to other embodiments, the Weyl-semimetal 55 may be a Diracmetal. Such a Dirac metal turns into a Weyl semimetal by the applicationof the magnetic field B. Such a Dirac metal may be e.g. Cd2As3 or Na3Bi.

According to other embodiments, the Weyl semimetal 55 may comprise RPtBior GdPtBi. These materials turn also into a Weyl semimetal by applyingthe magnetic field B.

FIG. 3 illustrates a signal flow of an electrical signal 70 in the firstpair comprising the leads 50 a and 50 b. The electrical signal 70 ise.g. a signal that shall be transferred from the neuron 10 a to theneuron 10 d. Accordingly, it is desired that the electrical signal 70 isforwarded from the lead 50 a only to the lead 50 b. More particularly,according to embodiments of the invention any crosstalk of theelectrical signal 70 into the lead 51 b of the second pair shall beminimized and preferably completely avoided. The electrical signal 70may be in particular embodied as Weyl-fermions that are transported bythe leads 50 a, 50 b of the first pair.

FIG. 4 illustrates a signal flow of an electrical signal 71 in thesecond pair comprising the leads 51 a and 51 b. The electrical signal 71is e.g. a signal that shall be transferred from the neuron 10 c to theneuron 10 b. Accordingly, it is desired that the electrical signal 71 isforwarded from the lead 51 a only to the lead 51 b. More particularly,according to embodiments of the invention any crosstalk of theelectrical signal 71 into the lead 50 b of the first pair shall beminimized and preferably completely avoided. The electrical signal 71may be in particular embodied as Weyl-fermions that are transported bythe leads 51 a, 51 b of the second pair.

The separation of the two electrical signals 70, 71 is achieved by thedifferent magnetization directions of the Weyl semimetal 55. Moreparticularly, the first magnetization direction 60 of the leads 50 a, 50b of the first pair is parallel to the direction of propagation of theelectrical signal 70, i.e. the Weyl-fermions in the first pair of leads.And the second magnetization direction 61 of the leads 51 a, 51 b of thesecond pair is antiparallel to the direction of propagation of theelectrical signal 71, i.e. the Weyl-fermions in the second pair ofleads. As a result of such a different magnetization of the leads 50 a,50 b of the first pair and the leads 51 a, 51 b of the second pair, theleads 50 a, 50 b of the first pair are configured to transportWeyl-fermions of a first chirality and the leads 51 a, 51 b of thesecond pair are configured to transport Weyl-fermions of a secondchirality. According to embodiments, the first chirality is aright-handed chirality and the second chirality is a left-handedchirality. According to other embodiments, the second chirality is aright-handed chirality and the first chirality is a left-handedchirality.

The chirality may be defined as the product of the spin of theWeyl-fermions and the direction of propagation of the Weyl-fermions.

Between the leads 50 a, 50 b of the first pair and the leads 51 a, 51 bof the second pair a crossing angle φ is provided. The crossing angle φis according to preferred embodiments less than 30 degree and accordingto even more preferred embodiments less than 20 degree. Such rathersmall crossing angles facilitate an efficient separation of theelectrical signals 70 and 71 and reduce and/or minimize any crosstalkbetween the different pairs of leads.

According to preferred embodiments, the crossing 30 provides a distanced₁ between the leads 50 a and 50 b of the first pair that issufficiently small to keep the first chirality of the Weyl-fermionsduring their transport through the crossing 30. The distance d₁ may bealso denoted as transport length.

Furthermore, according to preferred embodiments, the crossing 30provides a distance d₂ between the leads 51 a and 51 b of the secondpair that is sufficiently small to keep the second chirality of theWeyl-fermions during their transport through the crossing 30. Thedistance d₂ may be also denoted as transport length.

According to embodiments the distance d₁ between the leads 50 a and 50 bof the first pair and the distance d₂ between the leads 51 a, 51 b ofthe second pair is between 100 nm and 300 nm.

According to the embodiment of FIGS. 3 and 4, the crossing 30 has acircular shape. However, according to other embodiments other shapes maybe provided, e.g. hexagonal or octagonal shapes or other suitableshapes.

The material of the crossing 30 may be according to embodiments ametallic material. According to preferred embodiments the material ofthe crossing may be a non-magnetized Weyl-semimetal.

FIG. 5 shows an electrical junction 500 according to an embodiment ofthe invention.

The electrical junction 500 comprises a first pair of leads comprising alead 50 a and a lead 50 b. Furthermore, the electrical junction 500comprises a second pair of leads comprising a lead 51 a and a lead 51 b.The leads 50 a, 50 b as well as the leads 51 a and 51 b each comprise aWeyl semimetal 55. An electrical crossing 30 is arranged between theleads 50 a, 50 b of the first pair and the leads 51 a, 51 b of thesecond pair.

The first pair 50 of leads 50 a, 50 b comprises first magnetizedelements 80 which are arranged adjacent to the Weyl-semimetal of thefirst pair of leads 50 a, 50 b. The magnetized elements 80 apply adirected magnetic field B in the first magnetization direction 60 on theWeyl-semimetal 55 of the first pair of leads 50 a, 50 b. The magnetizedelements 80 are electrically insulated from the Weyl semimetal 55 by aninsulating layer 65.

The second pair of leads 51 a, 51 b comprises second magnetized elements81 which are arranged adjacent to the Weyl-semimetal of the second pairof leads 51 a, 51 b. The magnetized elements 81 apply a directedmagnetic field B in the second magnetization direction 61 on theWeyl-semimetal of the second pair of leads 51 a, 51 b.

The magnetized elements 81 are electrically insulated from the Weylsemimetal 55 by an insulating layer 65.

Accordingly, the Weyl semimetal 55 of the leads 50 a, 50 b of the firstpair is magnetized in the first magnetization direction 60 and the Weylsemimetal of the leads 51 a, 51 b of the second pair is magnetized inthe second magnetization direction 61.

According to embodiments, the first magnetized elements 80 and thesecond magnetized elements 81 may comprise rare earth magnets. Accordingto other embodiments, the magnetized elements 80, 81 may compriseNeodymium-iron-boron, mangan aluminum, samarium cobalt or aluminumnickel cobalt.

FIG. 6 shows an electrical junction 600 according to an embodiment ofthe invention.

The electrical junction 600 comprises a first pair of leads comprising alead 50 a and a lead 50 b. Furthermore, the electrical junction 600comprises a second pair of leads comprising a lead 51 a and a lead 51 b.The leads 50 a, 50 b as well as the leads 51 a and 51 b each comprise aWeyl semimetal 55. The Weyl semimetal 55 is illustrated with agrey-shading. An electrical crossing 30 is arranged between the leads 50a, 50 b of the first pair and the leads 51 a, 51 b of the second pair.

The first pair of leads 50 a, 50 b comprises a plurality of firstmagnetized elements 80 which are embedded in the Weyl semimetal of theleads 50 a, 50 b. The first magnetized elements 80 are illustrated withwhite dots in FIG. 6. The embedded magnetized elements 80 may be inparticular atoms. The embedded magnetized elements 80 may be integratedinto the Weyl-semimetal e.g. by magnetic doping techniques. Themagnetized elements 80 apply a directed magnetic field B in the firstmagnetization direction 60 on the Weyl-semimetal of the first pair ofleads 50 a, 50 b.

The second pair of leads 51 a, 51 b comprises a plurality of secondmagnetized elements 81 which are embedded in the Weyl semimetal of theleads 51 a, 51 b. The second magnetized elements 81 are illustrated withwhite dots in FIG. 6. The embedded magnetized elements 81 may be inparticular atoms. The embedded magnetized elements 81 may be integratedinto the Weyl-semimetal e.g. by magnetic doping techniques. The secondmagnetized elements 81 apply a directed magnetic field B in the secondmagnetization direction 61 on the Weyl-semimetal of the second pair ofleads 51 a, 51 b.

FIG. 7 shows a top view of an electrical junction 700 according to anembodiment of the invention.

The electrical junction 700 comprises a first pair of leads comprising alead 50 a and a lead 50 b. Furthermore, the electrical junction 700comprises a second pair of leads comprising a lead 51 a and a lead 51 b.The leads 50 a, 50 b as well as the leads 51 a and 51 b each comprise aWeyl semimetal. An electrical crossing 30 is arranged between the leads50 a, 50 b of the first pair and the leads 51 a, 51 b of the secondpair.

FIG. 8a shows a corresponding cross-sectional view of the first pair andthe crossing 30 taken along the section line I-I of FIG. 7.

FIG. 8b shows a corresponding cross-sectional view of the second pairand the crossing 30 taken along the section line II-II of FIG. 7.

The first pair of leads 50 a, 50 b comprises first magnetized elements80 which are embodied as magnetized layers and are arranged on top ofthe Weyl semimetal 55 of the first pair of leads 50 a, 50 b. Aninsulating layer 65 is provided between the first magnetized elements 80and the Weyl semimetal 55. The first magnetized elements 80 apply adirected magnetic field B in the first magnetization direction 60 on theWeyl-semimetal 55 of the first pair of leads 50 a, 50 b.

The second pair of leads 51 a, 51 b comprises second magnetized elements81 which are also embodied as magnetized layers and are arranged on topof the Weyl semimetal 55 of the second pair of leads 51 a, 51 b. Aninsulating layer 65 is provided between the second magnetized elements81 and the Weyl semimetal 55. The second magnetized elements 81 apply adirected magnetic field B in the second magnetization direction 61 onthe Weyl-semimetal 55 of the second pair of leads 51 a, 51 b.

FIG. 9 shows a cross-sectional view of another embodiment of anelectrical junction, taken along the section line I-I of FIG. 7. Theelectrical junction according to this embodiment comprises a lead 50 aof the first pair of leads and a lead 50 b of the first pair which arearranged in different vertical layers, i.e. in a different verticalpositions in the vertical z-direction. More particularly, the lead 50 ais arranged in a vertical layer VL1 and the lead 50 b in a verticallayer VL2. In other words, the lead 50 b is arranged in a higher layerabove the lead 50 a with respect to the vertical z-direction.

The descriptions of the various embodiments of the present inventionhave been presented for purposes of illustration, but are not intendedto be exhaustive or limited to the embodiments disclosed. Manymodifications and variations will be apparent to those of ordinary skillin the art without departing from the scope and spirit of the describedembodiments. The terminology used herein was chosen to best explain theprinciples of the embodiments, the practical application or technicalimprovement over technologies found in the marketplace, or to enableothers of ordinary skill in the art to understand the embodimentsdisclosed herein.

What is claimed is:
 1. An electrical junction comprising: a first pairof leads comprising a Weyl semimetal; a second pair of leads comprisinga Weyl semimetal; and an electrical crossing arranged between the leadsof the first pair and the leads of the second pair and configured toprovide an electrical connection between the leads of the first pair andthe leads of the second pair.
 2. An electrical junction according toclaim 1, wherein the Weyl semimetal of the leads of the first pair ismagnetized in a first magnetization direction and the Weyl semimetal ofthe leads of the second pair is magnetized in a second magnetizationdirection, the second magnetization direction being different from thefirst magnetization direction.
 3. An electrical junction according toclaim 2, wherein the first pair of leads and the second pair of leadsare configured to transport Weyl-fermions; the first magnetizationdirection is parallel to a direction of propagation of the Weyl-fermionsin the first pair of leads; and the second magnetization direction isantiparallel to the direction of propagation of the Weyl-fermions in thesecond pair of leads.
 4. An electrical junction according to claim 1,wherein the first pair of leads is configured to transport Weyl-fermionsof a first chirality; and the second pair of leads is configured totransport Weyl-fermions of a second chirality.
 5. An electrical junctionaccording to claim 2, wherein the first pair of leads comprises aplurality of first magnetized elements being configured to apply adirected magnetic field in the first magnetization direction on theWeyl-semimetal of the first pair of leads; and the second pair of leadscomprises a plurality of magnetized elements being configured to apply adirected magnetic field in the second magnetization direction on theWeyl-semimetal of the second pair of leads.
 6. An electrical junctionaccording to claim 5, wherein the plurality of first magnetized elementsand the plurality of second magnetized elements are arranged adjacent tothe Weyl-semimetal of the first pair of leads and adjacent to the Weylsemimetal of the second pair of leads respectively.
 7. An electricaljunction according to claim 5, wherein the plurality of first magnetizedelements are embodied as magnetized layers and/or the plurality ofsecond magnetized elements are embodied as magnetized layers.
 8. Anelectrical junction according to claim 5, wherein the plurality of firstmagnetized elements are embedded in the Weyl semimetal of the first pairof leads and the plurality of second magnetized elements are embedded inthe Weyl semimetal of the second pair of leads.
 9. An electricaljunction according to claim 1, wherein the leads of the first pair ofleads and/or the leads of the second pair of leads are arranged indifferent vertical layers.
 10. An electrical junction according to claim5, wherein the plurality of first magnetized elements and/or theplurality of second magnetized elements comprise rare earth magnets. 11.An electrical junction according to claim 5, wherein the plurality offirst magnetized elements and/or the plurality of second magnetizedelements comprise a material selected from the group consisting of:Neodymium-iron-boron, manganese aluminum, samarium cobalt and aluminumnickel cobalt.
 12. An electrical junction according to claim 1, whereinthe Weyl-semimetal is selected from the group consisting of: TaAs, NbP,TaP, RPtBi and GdPtBi.
 13. An electrical junction according to claim 1,wherein the Weyl-semimetal is a Dirac metal.
 14. An electrical junctionaccording to claim 13, wherein the Dirac metal is selected from thegroup consisting of: Cd₂As₃ and Na₃Bi.
 15. An electrical junctionaccording to claim 1, wherein a crossing angle between the leads of thefirst pair and the leads of the second pair is less than 30 degree, inparticular less than 20 degree.
 16. An electrical junction according toclaim 4, wherein the crossing is configured to provide a distancebetween the leads of the first pair that is sufficiently small to keepthe first chirality of the Weyl-fermions during their transport throughthe crossing; and to provide a distance between the leads of the secondpair that is sufficiently small to keep the second chirality of theWeyl-fermions during their transport through the crossing.
 17. Anelectrical junction according to claim 1, wherein the crossing isconfigured to provide a distance between the leads of the first pair andthe leads of the second pair between 50 nm and 300 nm.
 18. An electricaljunction according to claim 1, wherein the crossing comprises anon-magnetized Weyl-semimetal.
 19. An electrical device comprising aplurality of junctions according to claim
 1. 20. A neural networkcomprising: a plurality of neurons; a plurality of connections betweenthe neurons; and a plurality of junctions according to claim 1configured to provide a plurality of crossings between the plurality ofconnections.